Research/Sitter/MAGNDATA / 1.357_Ho3Ge4.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Ho3Ge4Spin lattice of Ho3Ge4

Ho3Ge4

MAGNDATA entry 1.357 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 6.6 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPc 21/c BNS 14.82
Point group2/m1′
Parent space groupC m c m No. 63
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1 0] 1k
Cella 4.0055 · b 10.543 · c 14.105 Å · α 90° · β 90° · γ 90°
Transition6.6 K (−267 °C)
Measured at1.4 K
Magnetic ionsHo
Largest moment component8.9 μB
MethodNPD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in Pc 21/c →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho00.33230.09700−8.98.9
Ho2Ho00.0440.257.2007.2
Ge1Ge00.3810.889
Ge2Ge00.7710.25
Ge3Ge000

Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

O. Zaharko et al. J. Phys.: Condens. Matter (1998) · doi:10.1088/0953-8984/10/29/015

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.357_Ho3Ge4.mcif from MAGNDATA · entry page

sha256 of this copy: 8eab4331d76f5d1a99d81d156c84811abcdd775ff8c0afce95b28b64eeea2ac5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.357_Ho3Ge4.mcif.